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研究了纯石墨和铜-石墨材料的阴极斑点的特性及真空电弧截流现象.发现纯石墨的阴极斑点呈现随机运动的特点,斑点的直径小于3μm,阴极斑点每次运动的距离约为阴极斑点的半径.而铜-石墨的阴极斑点的运动与Cu相息息相关,它选择性的发生在Cu相上,阴极斑点的大小取决于Cu相的大小,阴极斑点的运动距离为Cu相之间的距离.同时,铜-石墨的真空电弧截流值1.18 A,远远大于纯石墨的截流值,这主要是由于两种材料不同的阴极斑点运动特性引起的.

参考文献

[1] Jüttner B .[J].Journal of Physics D:Applied Physics,2001,34:R103.
[2] Djakov BE.;Juttner B. .Random and directed components of arc spot motion in vacuum[J].Journal of Physics, D. Applied Physics: A Europhysics Journal,2002(20):2570-2577.
[3] 段文新,郭聪慧,杨志懋,丁秉钧.CuCr触头材料小电流下阴极斑点与截流值研究[J].稀有金属材料与工程,2005(06):998-1001.
[4] DjakovBE;HolmesR .[J].J Phys D:Mppl Phys,1971,4:504.
[5] Peter R;Smeet P .[J].IEEE Trans Plasma & Sci,1989,17(02):303.
[6] 王发展 .旋锻法制备纳米复合W-ThO<,2>电极材料的研究[D].西安交通大学,2003.
[7] Ding B;Yang Z;Wang X .[J].IEEE Trans Comp,Package,Manufact Technol,1996,19(01):76.
[8] Restrepo E;Garcia LA;Castro JJ;Devia A .Craters formation in a graphite cathode produced by pulsed arc at low pressure[J].Applied Surface Science: A Journal Devoted to the Properties of Interfaces in Relation to the Synthesis and Behaviour of Materials,2005(5):1276-1282.
[9] Zhang CY.;Yang ZM.;Wang YP.;Ding BJ. .A worm-like trace of cathode spots on Cu-Zr-Ti amorphous ribbons[J].Journal of Physics, D. Applied Physics: A Europhysics Journal,2003(18):2276-2280.
[10] Marakhtanov M K;Marakhtanov A M .[J].Technical Physics Letters,1998,24(07):504.
[11] Beilis I I .[J].IEEE Transactions on Plasma Science,2001,29(05):657.
[12] 苏亚凤,杨志懋,丁秉钧.纳米Cu阴极斑点短程有向运动分析[J].稀有金属材料与工程,2007(01):68-70.
[13] 宋华,王新刚,冯宇,王茂林,丁秉钧.溶胶-凝胶法制备纳米复合Mo-La2O3阴极[J].稀有金属材料与工程,2005(10):1601-1604.
[14] 承欢;江剑平.阴极电子学[M].Xi'an:Xi'an Institute of Telecommunication Engineering Press,1986
[15] Dean J A.2004 Lange's Handbook of Chemistry[M].Ohio:McGraw-Hill Professional,2004:480.
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